3,106 research outputs found

    Ultra-compact structure in intermediate-luminosity radio quasars: building a sample of standard cosmological rulers and improving the dark energy constraints up to z3z\sim 3

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    In this paper, we present a new compiled milliarcsecond compact radio data set of 120 intermediate-luminosity quasars in the redshift range 0.46<z<2.760.46< z <2.76. These quasars show negligible dependence on redshifts and intrinsic luminosity, and thus represents, in the standard model of cosmology, a fixed comoving-length of standard ruler. We implement a new cosmology-independent technique to calibrate the linear size of of this standard ruler as lm=11.03±0.25l_m= 11.03\pm0.25 pc, which is the typical radius at which AGN jets become opaque at the observed frequency ν2\nu\sim 2 GHz. In the framework of flat Λ\LambdaCDM model, we find a high value of the matter density parameter, Ωm=0.3220.141+0.244\Omega_m=0.322^{+0.244}_{-0.141}, and a low value of the Hubble constant, H0=67.67.4+7.8  kms1Mpc1H_0=67.6^{+7.8}_{-7.4}\; \rm{kms}^{-1}\rm{Mpc}^{-1}, which is in excellent agreement with the CMB anisotropy measurements by \textit{Planck}. We obtain Ωm=0.3090.151+0.215{\Omega_m}=0.309^{+0.215}_{-0.151}, w=0.9701.730+0.500w=-0.970^{+0.500}_{-1.730} at 68.3% CL for the constant ww of a dynamical dark-energy model, which demonstrates no significant deviation from the concordance Λ\LambdaCDM model. Consistent fitting results are also obtained for other cosmological models explaining the cosmic acceleration, like Ricci dark energy (RDE) or Dvali-Gabadadze-Porrati (DGP) brane-world scenario. While no significant change in ww with redshift is detected, there is still considerable room for evolution in ww and the transition redshift at which ww departing from -1 is located at z2.0z\sim 2.0. Our results demonstrate that the method extensively investigated in our work on observational radio quasar data can be used to effectively derive cosmological information. Finally, we find the combination of high-redshift quasars and low-redshift clusters may provide an important source of angular diameter distances, considering the redshift coverage of these two astrophysical probes.Comment: 36 pages, 5 tables, 16 figures, A&A, in pres

    Association of glycemic variability and the presence and severity of coronary artery disease in patients with type 2 diabetes

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    <p>Abstract</p> <p>Background</p> <p>Glucose variability is one of components of the dysglycemia in diabetes and may play an important role in development of diabetic vascular complications. The objective of this study was to assess the relationship between glycemic variability determined by a continuous glucose monitoring (CGM) system and the presence and severity of coronary artery disease (CAD) in patients with type 2 diabetes mellitus (T2DM).</p> <p>Methods</p> <p>In 344 T2DM patients with chest pain, coronary angiography revealed CAD (coronary stenosis ≥ 50% luminal diameter narrowing) in 252 patients and 92 patients without CAD. Gensini score was used to assess the severity of CAD. All participants' CGM parameters and biochemical characteristics were measured at baseline.</p> <p>Results</p> <p>Diabetic patients with CAD were older, and more were male and cigarette smokers compared with the controls. Levels of the mean amplitude of glycemic excursions (MAGE) (3.7 ± 1.4 mmol/L vs. 3.2 ± 1.2 mmol/L, p < 0.001), postprandial glucose excursion (PPGE) (3.9 ± 1.6 mmol/L vs. 3.6 ± 1.4 mmol/L, p = 0.036), serum high-sensitive C-reactive protein (hs-CRP) (10.7 ± 12.4 mg/L vs. 5.8 ± 6.7 mg/L, p < 0.001) and creatinine (Cr) (87 ± 23 mmol/L vs. 77 ± 14 mmol/L, p < 0.001) were significantly higher in patients with CAD than in patients without CAD. Gensini score closely correlated with age, MAGE, PPGE, hemoglobin A<sub>1c </sub>(HbA<sub>1c</sub>), hs-CRP and total cholesterol (TC). Multivariate analysis indicated that age (p < 0.001), MAGE (p < 0.001), serum levels of HbA<sub>1c </sub>(p = 0.022) and hs-CRP (p = 0.005) were independent determinants for Gensini score. Logistic regression analysis revealed that MAGE ≥ 3.4 mmol/L was an independent predictor for CAD. The area under the receiver-operating characteristic curve for MAGE (0.618, p = 0.001) was superior to that for HbA<sub>1c </sub>(0.554, p = 0.129).</p> <p>Conclusions</p> <p>The intraday glycemic variability is associated with the presence and severity of CAD in patients with T2DM. Effects of glycemic excursions on vascular complications should not be neglected in diabetes.</p

    catena-Poly[[diaqua­[(4-tolyl­sulfan­yl)acetato-κO]cadmium(II)]-μ-4,4′-bipyridine-κ2 N:N′]

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    The title complex, [Cd(C9H9O2S)2(C10H8N2)(H2O)2]n, has a linear chain structure. The central CdII ion is in a slightly disorted octa­hedral environment, coordinated by two aqua ligands, two (4-tolyl­sulfan­yl)acetate ligands and two bridging 4,4′-bipyridine ligands. The CdII ion lies on a twofold rotation axis. Inter­molecular O—H⋯O hydrogen bonds connect adjacent chains, forming a layer structure. An intramolecular O—H⋯O hydrogen bond is also present

    On leptonic width of X(4260)X(4260)

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    New measurements on cross sections in e+eJ/ψπ+πe^+e^-\to J/\psi\pi^+\pi^-, hcπ+πh_c\pi^+\pi^-, D0Dπ++c.c.D^0D^{*-}\pi^++c.c., ψ(2S)π+π\psi(2S)\pi^+\pi^-, ωχc0\omega\chi_{c0} and J/ψηJ/\psi\eta channels have been carried out by BESIII, Belle and BABAR collaborations, and also in the DsDˉsD_s^*\bar D_s^* channel. We perform extensive numerical analyses by combining all these data available, together with those in DDˉD\bar D^* and DDˉD^*\bar D^* channels. Though the latter show no evident peak around s=4.230\sqrt{s}=4.230 GeV, the missing X(4260)X(4260) is explained as that it is concealed by the interference effects of the well established charmonia ψ(4040)\psi(4040), ψ(4160)\psi(4160) and ψ(4415)\psi(4415). Our analyses reveal that the leptonic decay width of X(4260)X(4260) ranges from O(102)O(10^2) eV to O(1)O(1) keV, and hence may be explained in the conventional quark model picture. That is, the X(4260)X(4260) may well be interpreted as a mixture of 43S14^3S_1 and 33D13^3D_1 states.Comment: two small mistakes are fixed, figures redrawn, major physical outputs remain unchanged. Version published in EPJ
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